Method of assembling tire and wheel, recording medium which records phase angle operating program at the time of assembling tire and wheel, and assembled tire and wheel unit

ABSTRACT

An unbalance mass at the front side of a single wheel unit, an unbalance mass at the reverse side of the single wheel unit, a phase difference between the unbalance mass at the front side and the unbalance mass at the reverse side of the single wheel unit, a primary component amplitude of radial run-out of the single wheel unit, a phase angle of the primary component of the radial run-out of the single wheel unit, a contribution coefficient in which the radial run-out of the single wheel unit is transmitted to an RFV, an unbalance mass at the front side of a single tire unit, an unbalance mass at the reverse side of the single tire unit, a phase difference between the unbalance mass at the front side and the unbalance mass at the reverse side of the single tire unit, an RFV primary component amplitude of the single tire unit, and a phase angle of the RFV primary component of the single tire unit are measured and the measured values are input. Evaluation functions for evaluating an optimum assembling angle of the tire and the wheel in accordance with an object are determined, and the optimum assembling angle is determined and output as a predicted angle using the determined evaluation functions.

This is a Division of application Ser. No. 09/263,946 filed Mar. 8, 1999, the disclosure of which is incorporated herein by reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a method of assembling a tire and a wheel, a recording medium which records a phase angle operating program at the time of assembling a tire and a wheel, and an assembled tire and wheel unit. More particularly, the present invention relates to method of assembling a tire and a wheel, a recording medium which records a phase angle operating program at the time of assembling a tire and a wheel for obtaining an optimum phase angle at the time of assembling the tire and the wheel as a predicted angle, and an assembled tire and wheel unit which is assembled in accordance with the method of assembling a tire and a wheel.

2. Description of the Related Art

Conventionally, in order to prevent vibrations of a vehicle caused by unevenness on the peripheries of a tire and a wheel due to the irregularities at the time of manufacturing the single wheel unit and the single tire unit, a positional relationship between the wheel and the tire during assemble is intentionally selected and the assembling is effected in the positional relationship. The typical method is called radial force variation (RFV) primary matching. In this assembling method, a bottom position of a Fourier primary component of radial direction vibrations (radial run-out, the mean of the front side/reverse side of the wheel) of a single wheel unit and a peak position of an RFV primary component of a single tire are matched. This is because the RFV primary component of the single tire unit after the assembling is expected to be reduced by the value of the RFV primary component caused by the vibrations of the single wheel unit.

In addition to RFV caused by the above-described small vibrations on the periphery of the tire or unevenness of rigidity, unevenness on the periphery of the tire is also caused by unevenness of mass distribution which is called unbalance. This unbalance generates centrifugal force when the assembled tire and wheel unit is rotated and causes vibrations in a vehicle by exciting an axle at the primary frequency of rotation. After the wheel and the tire are assembled, this unbalance can be theoretically cancelled by adding balance weights having accurate masses one by one to each of specific places of flange portions at the front and reverse sides of the wheel, and balancing is actually routinely effected by a method (two-surface balancing method) in accordance with this principle using a commercially-available wheel balancer.

In an operation for correcting the unevenness of the assembled wheel and tire unit to prevent the vibrations of a vehicle, basically, the two aforementioned procedures are effected in succession and the adjustment is completed when these procedures are completed. Namely, the wheel and the tire which have been adjusted are lightened by an amount corresponding to the run-out of the wheel due to the RFV primary matching of the single tire.

However, deviation (unbalance) in the entire mass distribution which is determined after the assembling may be generated on the assembled unit by the RFV primary matching, therefore a balance weight which matches the entire amount of the deviation to be rectified is forcibly added to the assembled body from an exterior.

In this way, in accordance with the RFV primary matching, the RFV of the tire is reduced using the radial direction vibrations of the wheel which is one type of unevenness of the wheel, and the wheel and the tire are thereby assembled. The unbalance accompanying the assembling method is corrected by adding the balance weight, and the assembled tire and wheel unit is obtained.

However, the amount of balance weight required for correcting the unbalance is determined by the amounts of unbalance of the wheel and the tire and the positional relationship therebetween. As a result, in the uniform assembling of the wheel and the tire called the RVF primary matching, the effect of reducing RFV is small and the amount of balance weight is excessively large. In extreme cases, when the position of a wheel, whose vibrations are very small but which has a reasonable amount of unbalance, coincidentally matches perfectly the unbalance position of the tire at the time of effecting the assembling by the RFV primary matching, the absurd outcome is that the assembling method, in which the effect of reducing RFV is almost zero and the unbalance is the worst, ends up being intentionally selected.

Further, the excessively large balance weight is not preferable because of its appearance and is counter-productive to reducing the weight of the tire. Moreover, lead has been mainly used for the balance weight, however, since the use of lead is banned for social reasons such as environmental problems or the like, iron is considered as the alternative balance weight. Nevertheless, since the specific gravity of iron is smaller than that of lead, the volume per weight thereof increases. Thus, it is desirable that the amount of unbalance itself is reduced.

SUMMARY OF THE INVENTION

With the aforementioned in view, an object of the present invention is to obtain a method of assembling a tire and a wheel which can reduce the amount of unbalance, a recording medium which records a phase angle operating program at the time of assembling the tire and the wheel, and an assembled tire and wheel unit.

In order to achieve the above-described object, a first aspect of the present invention is a method of assembling a tire and a wheel, comprising the steps of: on the basis of a physical amount of unbalance which includes the magnitude and the position of the amount of unbalance of a tire and the magnitude and the position of the amount of unbalance of a wheel for assembling with the tire, obtaining a predicted angle for assembling the tire and the wheel using a predetermined evaluation function for evaluating the relationship between the tire and the wheel at the time of assembly; and assembling the tire and the wheel at the predicted angle.

A second aspect of the present invention is a method of assembling a tire and a wheel, comprising the steps of: on the basis of a physical amount of unbalance which includes the magnitude of the amount of unbalance on the axial direction end surfaces of a tire, the position of the amount of unbalance on the periphery of the end surface of the tire, the magnitude of the amount of unbalance on the axial direction end surfaces of a wheel for assembling with the tire, and the position of the amount of unbalance on the periphery of the end surface of the wheel, obtaining a predicted angle for assembling the tire and the wheel using a predetermined evaluation function which includes the phase angle at the time of assembling the tire and the wheel for evaluating the relationship between the tire and the wheel at the time of assembly; and assembling the tire and the wheel at the predicted angle.

A third aspect of the present invention is a method of assembling a tire and a wheel according to the first aspect or the second aspect of the present invention, wherein the evaluation function indicates the magnitude of the amount of static unbalance correction after the tire and the wheel are assembled.

A fourth aspect of the present invention is a method of assembling a tire and a wheel according to the second aspect of the present invention, wherein the evaluation function indicates the magnitude of at least one of the amounts of unbalance correction on the axial direction end surfaces of the wheel after the tire and the wheel are assembled.

A fifth aspect of the present invention is a method of assembling a tire and a wheel according to the second aspect of the present invention, wherein the physical amount of unbalance further includes a physical amount relating to radial direction vibrations of the tire and a physical amount relating to radial direction vibrations of the wheel, and the evaluation function indicates the physical amounts relating to the radial direction vibrations of the tire and the wheel after the tire and the wheel are assembled.

A sixth aspect of the present invention is a method of assembling a tire and a wheel according to the second aspect of the present invention, wherein the physical amount of unbalance further includes a physical amount relating to radial direction vibrations of the tire and a physical amount relating to radial direction vibrations of the wheel, and the evaluation function indicates the sum of the physical amount of the magnitude of at least one of the amounts of unbalance correction on the axial direction end surfaces of the wheel after the wheel and the tire are assembled and a weight is attached thereto, and the physical amount relating to the radial direction vibrations of the wheel and the tire after the tire and the wheel are assembled and a weight is attached thereto.

A seventh aspect of the present invention is a method of assembling a tire and a wheel according to the second aspect of the present invention, wherein the physical amount of unbalance further includes a physical amount relating to radial direction vibrations of the tire and a physical amount relating to radial direction vibrations of the wheel, and the evaluation function indicates, in a predetermined relationship, the physical amount of the magnitude of at least one of the amounts of unbalance correction on the axial direction end surfaces of the wheel after the wheel and the tire are assembled and a weight is attached thereto, and the physical amount relating to the radial direction vibrations of the wheel and the tire after the wheel and the tire are assembled and a weight is attached thereto.

An eighth aspect of the present invention is a method of assembling a tire and a wheel according to any one of the first through seventh aspects of the present invention, wherein a valve for intaking air is attached to the wheel.

A ninth aspect of the present invention is a method of assembling a tire and a wheel according to any one of the first through eighth aspects of the present invention, wherein the physical amount relating to radial direction vibrations of the wheel is radial run-out, and the physical amount relating to radial direction vibrations of the tire is at least one uniformity of radial force variation and lateral force variation.

A tenth aspect of the present invention is a record medium which records a phase angle operating program at the time of assembling a tire and a wheel in which an optimum phase angle at the time of assembling the tire and the wheel is obtained by a computer as a predicted angle, wherein: a physical amount of unbalance which includes the magnitude of the amount of unbalance on the axial direction end surfaces of a tire, the position of the amount of unbalance on the periphery of the end surface of the tire, the magnitude of the amount of unbalance on the axial direction end surfaces of a wheel for assembling with the tire, and the position of the amount of unbalance on the periphery of the end surface of the wheel is measured; and a predicted angle for assembling the tire and the wheel is obtained on the basis of the physical amount of unbalance using a predetermined evaluation function which includes a phase angle at the time of assembling the tire and the wheel for evaluating a relationship between the tire and the wheel at the time of assembly.

An eleventh aspect of the present invention is an assembling body of a tire and a wheel, wherein: a physical amount of unbalance which includes the magnitude of the amount of unbalance on the axial direction end surfaces of a tire, the position of the amount of unbalance on the periphery of the end surface of the tire, the magnitude of the amount of unbalance on the axial direction end surfaces of a wheel for assembling with the tire, and the position of the amount of unbalance on the periphery of the end surface of the wheel is measured; a predicted angle for assembling the tire and the wheel is obtained on the basis of the physical amount of unbalance using a predetermined evaluation function which includes a phase angle at the time of assembling the tire and the wheel for evaluating the relationship between the tire and the wheel at the time of assembly; and the tire and the wheel are assembled at the predicted angle.

In the first and second aspects of the present invention, on the basis of the physical amount of unbalance which includes the magnitude and the position of the amount of unbalance of the tire and the magnitude and the position of the amount of unbalance of the wheel for assembling with the tire, the predicted angle for assembling the tire and the wheel is obtained using the predetermined evaluation function for evaluating the relationship between the tire and the wheel at the time of assembly. The tire and the wheel are assembled at this predicted angle.

The magnitudes and the positions of the amounts of unbalance of the tire and the wheel, which comprises the physical amount of unbalance, can be obtained by measuring or can be obtained using values which have been already measured. This physical amount of unbalance includes, for example, the magnitude and the phase (position) of a static unbalance, and the evaluation function can use the static unbalance after the tire and the wheel are assembled. Normally, it is desirable that the static unbalance is made small. When the single tire unit and the single wheel unit are assembled so that each phase (position) of the static unbalance thereof is 180 degrees, it can be expected that the amount of static unbalance after the tire and the wheel are assembled will be reduced. Accordingly, the amount of unbalance to be corrected can be made as small as possible at the time of assembling the wheel and the tire, and the magnitude of the balance weight which should be the magnitude of the amount of unbalance to be corrected after the wheel and the tire are assembled can be reduced. Consequently, even if iron whose specific gravity is smaller than that of lead which has been conventionally used is used, the amount of unbalance itself can be reduced. Thus, correction of unbalance can be effected without increasing the volume of the iron used.

Therefore, in accordance with the third aspect of the present invention, when an evaluation function which indicates the magnitude of the amount of static unbalance correction after the tire and the wheel are assembled is used, and the tire and the wheel are assembled at the predicted angle of, for example, 180 degrees which can optimize the amount of unbalance to be corrected, the balance weight for correcting the unbalance can be made small.

The phase (position) can be set to 180 degrees, the value which is in the vicinity of 180 degrees, or a predetermined range. The evaluation function may be determined so that the amount of static unbalance after the assembling is a predetermined value.

The physical amount of unbalance can include the magnitude of the amount of unbalance on the axial direction end surfaces of the tire, the position of the amount of unbalance on the periphery of the end surface of the tire, the magnitude of amount of unbalance on the axial direction end surfaces of the wheel for assembling with the tire and the position of the amount of unbalance on the periphery of the end surface of the wheel.

On the basis of these physical amounts of unbalance, the predicted angle for assembling the tire and the wheel is obtained using the predetermined evaluation function which includes the phase angle at the time of assembling the tire and the wheel for evaluating the relationship between the tire and the wheel at the time of assembly. In this case, the deviated angle at the time in which the predetermined reference positions on the peripheries of the tire and the wheel are deviated from each other and assembled is the phase angle at the time of assembling the tire and the wheel, and the phase angle is used as a parameter. The relationship between the tire and the wheel at the time of assembly is evaluated and, for example, the magnitude or the like of the amount of unbalance to be corrected at the phase angle is obtained. The phase angle at the time of assembling the wheel and the tire which can optimize this evaluation function is predicted and the predicted phase angle is made the predicted angle. Then, the tire and the wheel are assembled by the obtained predicted angle.

In this way, since the tire and the wheel are assembled at the predicted angle which can optimize the evaluation function, the amount of unbalance to be corrected can be made as small as possible at the time of assembling the tire and the wheel, and the magnitude of a balance weight which should be the magnitude of the amount of unbalance to be corrected after the wheel and the tire are assembled can be reduced. Consequently, even if iron whose specific gravity is smaller than that of lead, which has been conventionally used, is used, the amount of unbalance to be corrected itself can be reduced. Thus, correction of unbalance can be effected without increasing the volume of the iron used.

Even when the amount of unbalance on the axial direction end surfaces of the tire and the amount of unbalance on the axial direction end surfaces of the wheel are used as the physical amount of unbalance, in accordance with the third aspect of the present invention, the evaluation function which indicates the magnitude of the amount of static unbalance to be corrected after the tire and the wheel are assembled can be used. In this way, when the tire and the wheel are assembled so that the phase formed by the amount of unbalance on the axial direction end surfaces of the wheel and the phase formed by the amount of unbalance on the axial direction end surfaces of the tire is, for example, 180 degrees which can optimize the amount of unbalance to be corrected, the balance weight for correcting the unbalance can be made small.

In accordance with the fourth aspect of the present invention, the evaluation function which indicates the magnitude of at least one of the amounts of unbalance to be corrected on the axial direction end surfaces of the wheel after the tire and the wheel are assembled can be used. The magnitude of the amount of unbalance to be corrected at the phase angle is obtained by this evaluation function. When the phase angle at the time of assembling the wheel and the tire which allows the amount of unbalance to be corrected to be optimized (e.g., which allows the magnitude of the balance weight to be reduced, which allows the magnitude of the balance weight to be set to a predetermined value, or which allows the magnitude of the balance weight to be set to a value within a predetermined range) is set as a predicted angle and the tire and the wheel are assembled at the predicted angle, the amount of unbalance to be corrected is reduced and the balance weight for correcting the unbalance can be made small.

In accordance with the fifth aspect of the present invention, the physical amount of unbalance can further include the physical amount relating to the radial direction vibrations of the tire and the physical amount relating to the radial direction vibrations of the wheel. In this case, the evaluation function which indicates the physical amounts relating to the radial direction vibrations of the tire and the wheel after the tire and the wheel are assembled can be used. As a result, the phase angle which can optimize the amount of unbalance to be corrected, e.g., which can reduce the RFV primary component or the like after the wheel and the tire are assembled, can be obtained as the predicted angle. When the tire and the wheel are assembled at the predicted angle, the amount of unbalance to be corrected, e.g., the magnitude of the balance weight or the RFV primary component, can be made as small as possible, can be set to a predetermined value, or can be set to a value within a predetermined range. Thus, it is easy to assemble the wheel and the tire.

In accordance with the sixth aspect of the present invention, an evaluation function can be used which indicates the sum of the physical amount of the magnitude of at least one of the amounts of unbalance correction on the axial direction end surfaces of the wheel after the wheel and the tire are assembled and a weight is attached thereto, and the physical amount relating to the radial direction vibrations of the wheel and the tire after the tire and the wheel are assembled and a weight is attached thereto. Since the physical amounts are weighted in this way, the relationship between the tire and the wheel at the time of assembly can be evaluated by the linear sum of the amounts of unbalance. As a result, the amount of unbalance to be corrected, e.g., the magnitude of the balance weight, the RFV primary component, or the like, can be made as small as possible, can be set to a predetermined value, or can be set to a value within the predetermined range. Thus, the optimum phase angle at the time of assembling the tire and the wheel can be obtained.

Further, in accordance with the seventh aspect of the present invention, the weighted physical amounts of the evaluation function may have a predetermined relationship. In this way, the relationship is not limited to the evaluation by a linear sum and may be evaluated, e.g., by a non-linear function or the like. Moreover, a table which includes predetermined corresponding relationships on the physical amounts may be referred to and the physical amounts summed or calculated by a predetermined function to obtain the predetermined relationship. As a result, it is more flexible to, for example, reduce greatly the amount of unbalance to be corrected, e.g., the magnitude of the unbalance weight or the RFV primary component.

The air intake valve is attached to the wheel, and the weight of this air intake valve may contribute to the unbalance. Thus, in accordance with the eighth aspect of the present invention, the wheel, to which the valve for intaking air is attached, is used. As a result, the optimum phase angle for assembling the tire and the wheel, to which the actual air intake valve is attached, can be obtained.

In accordance with the ninth aspect of the present invention, the physical amount relating to the radial direction vibrations of the wheel can use the radial run-out, and the physical amount relating to the radial direction vibrations of the tire can use at least one uniformity of the radial force variation and the lateral force variation.

The predicted angle which is an optimum phase angle for assembling the tire and the wheel is obtained by a record medium which stores a phase angle operating program having the following procedures. The storage medium which stores the program is easily portable allowing the program to be used on-site when the tires and wheels are being assembled.

Namely, the recording medium which records the phase angle operating program of the tenth aspect of the present invention is the record medium which records the phase angle operating program at the time of assembling the tire and the wheel in which the optimum phase angle at the time of assembling the tire and the wheel is obtained by the computer as the predicted angle, wherein: the physical amount of unbalance which includes the magnitude of an amount of unbalance on the axial direction end surfaces of the tire, the position of an amount of unbalance on the periphery of the end surface of the tire, the magnitude of an amount of unbalance on the axial direction end surfaces of the wheel for assembling with the tire, and the position of an amount of unbalance on the periphery of the end surface of the wheel is measured; and the predicted angle for assembling the tire and the wheel is obtained on the basis of the physical amount of unbalance using the predetermined evaluation function which includes the phase angle at the time of assembling the tire and the wheel for evaluating the relationship between the tire and the wheel.

In accordance with the method of assembling the tire and the wheel in which the predicted angle of the tire and the wheel is obtained and the tire and the wheel are assembled at the predicted angle, the following assembled tire and wheel unit can be obtained. Namely, in accordance with the eleventh aspect of the present invention, the assembled tire and wheel unit, wherein: the physical amount of unbalance which includes the magnitude of an amount of unbalance on the axial direction end surfaces of the tire, the position of an amount of unbalance on the periphery of the end surface of the tire, the magnitude of an amount of unbalance on the axial direction end surfaces of the wheel for assembling with the tire, and the position of an amount of unbalance on the periphery of the end surface of the wheel is measured; the predicted angle for assembling the tire and the wheel is obtained on the basis of the physical amount of unbalance using the predetermined evaluation function which includes the phase angle at the time of assembling the tire and the wheel for evaluating the relationship between the tire and the wheel; and the tire and the wheel are assembled at the predicted angle.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a principle explanatory diagram for explaining the principle of the present invention pertaining to a wheel.

FIG. 2 is a principle explanatory diagram for explaining the principle of the present invention pertaining to a tire.

FIG. 3 is a principle explanatory diagram for explaining the principle of the present invention pertaining to an assembled tire and wheel unit.

FIG. 4 is a schematic view of a personal computer which is used in an embodiment of the present invention.

FIG. 5 is a flow chart showing a processing routine of the embodiment of the present invention.

FIG. 6A corresponds to Strategy 1 and shows the dispersion of simulation results of an assembled unit in which the tire and the wheel were assembled with the assembling angle θ determined using an evaluation function A (minimalization of n₁+n₂).

FIG. 6B corresponds to Strategy 2 and shows the dispersion of simulation results of an assembled unit in which the tire and the wheel were assembled with the assembling angle θ determined using an evaluation function B (minimalization of n₁).

FIG. 6C corresponds to Strategy 3 and shows the dispersion of simulation results of an assembled unit in which the tire and the wheel were assembled with the assembling angle θ determined using an evaluation function E (matching of RFV primary amplitude f).

FIG. 6D corresponds to no strategy and shows the dispersion of simulation results of an assembled unit in which the tire and the wheel were assembled with the assembling angle θ determined at random without using an evaluation function.

FIG. 6E shows the means of the simulation results of the respective strategies.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

An embodiment of the present invention will be explained in detail hereinafter with reference to the drawings.

First, the principle of the present invention will be explained.

The unbalances of a single wheel unit, a single tire unit, and an assembled tire and wheel unit will be described with reference to FIGS. 1 through 3.

As shown in FIG. 1, a wheel surface P is a surface (so-called equatorial plane) which is parallel to end surfaces (front and reverse surfaces) of a wheel for assembling with a tire and passes through a center O_(W). Further, as a result of measurement using an unbalance measuring machine which is used normally and widely for correcting unbalances simultaneously, it is assumed that an unbalance mass μ₁, which is a vector amount, is needed on the circumference of the front surface of the wheel (on the periphery of the end surface of the wheel), that an unbalance mass μ₂, which is a vector amount, is needed on the circumference of the reverse surface of the wheel, and that the unbalance masses μ₁ and μ₂ have a phase difference α_(W). These unbalance masses μ₁ and μ₂ are projected on the wheel surface P and will be explained hereinafter. Further, it is assumed that a radial run-out primary component Δr measured at the single wheel is disposed on the position of a phase angle β_(W) on the basis of the position of the unbalance mass μ₁.

As shown in FIG. 2, a tire surface Q is a surface (so-called equatorial plane) which is parallel to end surfaces (front and reverse surfaces) of a tire and passes through a center O_(T). Further, as a result of measurement using the unbalance measuring machine which is the same as the one described above, it is assumed that an unbalance mass m₁, which is a vector amount, is needed on the circumference of the front surface of the tire (on the periphery of the end surface of the wheel), that an unbalance mass m₂, which is a vector amount, is needed on the circumference of the reverse surface of the tire, and that the unbalance masses m₁ and m₂ have a phase difference α_(T). These unbalance masses m₁ and m₂ are projected on the tire surface Q and will be explained hereinafter. Further, it is assumed that an RFV primary component amplitude f₀ measured at the single tire is disposed on the position of a phase angle β_(T) on the basis of the position of the unbalance mass m₁.

As shown in FIG. 3, an assembled unit surface R is a surface (so-called equatorial plane) which is parallel to the end surfaces (front and reverse surfaces) of the assembled unit, in which the single wheel unit and the single tire unit which are defined as described above are assembled, and passes through a center O. Further, the wheel in FIG. 1 and the tire in FIG. 2 are assembled having an arbitrary assembling angle (phase angle) θ. This assembling angle θ is a counterclockwise assembling angle of the unbalance mass m₁ of the tire on the basis of the position of the unbalance mass μ₁ of the wheel.

Because the measured values of unbalances (two-surface balances) of the single wheel unit and the single tire unit and the measured values of the radial run-out primary component of the single wheel and the RFV primary component of the single tire are obtained, the amounts of unbalance and the RFV primary component at the time of assembling the wheel and tire in the arbitrary positional relationship (the assembling angle θ in FIG. 3) can be predicted as a function of the assembling angle θ. Namely, as described below, the amounts of unbalance and the RFV primary component can be predicted in formulas formed by vector compositions of forces corresponding to the above-described factors.

The amount of unbalance weight to be corrected n₁ at the front side of the assembled wheel can be expressed by the following formula (1).

n ₁={square root over (μ₁ ²+m ₁ ²+2 μ₁ m ₁ cosθ)}  (1)

The amount of unbalance weight to be corrected n₂ at the reverse side of the assembled wheel can be expressed by the following formula (2).

n ₂={square root over (μ₂ ²+m ₂ ²+2μ₂ m ₂ cos(θ+α_(T)−α_(W)))}  (2)

The amplitude f of the RFV primary component can be expressed by the following formula (3).

f={square root over (f ₀ ²+(kΔr)²+2f ₀(kΔr) cos(θ+β_(T)−β_(W)))}  (3)

wherein,

μ₁ is an unbalance mass at the front side of the single wheel unit;

μ₂ is an unbalance mass at the reverse side of the single wheel unit;

α_(W) is a phase difference between μ₁ and μ₂ (a counterclockwise angle from the position of μ₁ to the position of μ₂ when viewed from the front side);

m₁ is an unbalance mass at the front side of the single tire unit;

m₂ is an unbalance mass at the reverse side of the single tire unit;

α_(T) is a phase difference between m₁ and m₂ (a counterclockwise angle from the position of m₁ to the position of m₂ when viewed from the front side);

θ is a counterclockwise assembling angle from the position of μ₁ of the wheel to the position of m₁ of the tire;

Δr is a primary component amplitude of a radial run-out (front and reverse average waveform) of the single wheel unit;

k is a contribution coefficient in which the radial run-out of the single wheel unit is transmitted to the RFV;

β_(W) is a phase angle of Δr which is measured counterclockwisely from the position of μ₁;

f₀ is an RFV primary component amplitude of the single tire unit; and

β_(T) is a phase angle of f₀ which is measured counterclockwisely from the position of m₁.

Among the above-described parameters, only the contribution coefficient k is unknown. It is considered that this contribution coefficient k is an amount determined by the rigidity of the tire itself. More specifically, the difference between the RFV primary amplitude when the assembling is effected in accordance with the RFV primary matching and the RFV primary amplitude when the assembling is effected by shifting 180 degrees therefrom is halved and divided by Δr. The contribution coefficient k is thereby obtained. Since it is considered that this contribution coefficient k is a constant which is the same among tires having the same specifications, if the contribution coefficient k of one representative tire or tires having the same specifications is obtained in accordance with the above-described measurement, it is no longer necessary thereafter to measure the contribution coefficients k of respective tires and the obtained value can be used for prediction in the above formulas (1), (2), and (3).

Next, the above formulas (1), (2), and (3) will be explained in detail.

First, a description regarding the states of unbalance of a wheel and a tire will be explained. As it is clear that both the static unbalance and the dynamic unbalance of the wheel or the tire can be completely corrected by a balancer on the principle of two-plane balancing, the state of unbalance is the same as the state in which an extra mass which is the same as a correction weight exists (with respect to a completely balanced state) at a position substantially 180 degrees opposite the position on the front and reverse flange portion of the wheel at which the correction balance weight is to be added. Accordingly, the state of unbalance can be described by four parameters, i.e., {circle around (1)} an unbalance mass at the front side, {circle around (2)} an angle coordinate which shows the position at which the unbalance mass at the front side exists, {circle around (3)} an unbalance mass at the reverse side, {circle around (4)} an angle coordinate which shows the position at which the unbalance mass at the reverse side exists. Since the origin of the angle coordinate can be arbitrarily determined, if the position at which the unbalance mass at the front side exists in parameter {circle around (2)} is selected to be an origin, the parameter {circle around (2)} can be zero. The parameters which specify the states of unbalance of the wheel and the tire in the above formulas will be respectively given as (μ₁, 0, μ₂, α_(W)) and (m₁, 0, m₂, α_(T)). These are regarded as states of unbalance.

Next, when the wheel in the state of unbalance (μ₁, 0, μ₂, α_(W)) and the tire in the state of unbalance (m₁, 0, m₂, α_(T)) are assembled so that the position of the unbalance mass m₁ of the tire is disposed at the position of the angle which is counterclockwise from the position of the unbalance mass μ₁ of the wheel, the overall state of unbalance can be described by the similar four parameters and the state of unbalance is defied as (n₁, γ₁, n₂, γ₂) (wherein, the origin of the angle matches the position of the unbalance mass μ₁). A physical meaning of the state of unbalance (μ₁, 0, μ₂, α_(W)) or the like is that, when the wheel is rotated, centrifugal force which is proportional to the unbalance mass μ₁ is applied in the direction toward the position of the unbalance mass μ₁ from the wheel center at the front side of the wheel and that centrifugal force which is proportional to the unbalance mass μ₂ is applied in the direction of the reverse side (in the direction toward the position of the unbalance mass μ₂). The same is applied to the state of unbalance (m₁, 0, m₂, α_(T)). When the tire and the wheel are assembled, the resultant forces (i.e., the force of n₁) of the unbalance mass μ₁ and the unbalance mass m₁ are applied to the front side of the wheel and the resultant forces (i.e., the force of n₂) of the unbalance mass μ₂ and the unbalance mass m₂ are applied to the reverse side of the wheel. Accordingly, from the composition rule of forces, when these components of forces are expressed in a rectangular coordinate system in which the direction of unbalance mass μ₁ is X-axis and the direction 90 degrees counterclockwise from the X-axis is Y-axis, the following formulas are formed.

n ₁ cos γ₁=μ₁ +m ₁ cos θ  (4)

n ₁ sin γ₁ =m ₁ sin θ  (5)

n ₂ cos γ₂=μ₂ cos α_(W) +m ₂ cos (θ+α_(T))  (6)

n ₂ sin γ₂=μ₂ sin α_(W) +m ₂ sin (θ+α_(T))  (7)

The formula (1) is obtained by squaring, summing, and extracting the square root both sides of the above-described formulas (4) and (5). The formula (2) is obtained in the same way from the formulas (6) and (7).

Next, the formula (3) will be explained.

The principle of RFV primary matching is expressed in the formula (3). Namely, the RFV of the single tire unit is the one in which the tire is assembled with a wheel which has very high degree of roundness and is precisely manufactured. Because the RFV is not affected by the vibrations of the wheel, the value does not depend on the assembling angle. Consequently, since the phase is determined only by the coordinates fixed to the tire at the time of primary component amplitude f₀, the value of the primary component amplitude which is measured on the basis of the position of the unbalance mass m₁ is a phase angle β_(T). On the other hand, when the wheel which has a radial run-out in which a primary component amplitude is Δr and a phase angle is β_(W) in a wheel system is assembled to the tire, it is approximately considered that an additional RFV primary component of the wheel having an amplitude which is proportional to the primary component amplitude Δr (the proportional constant thereof is the aforementioned contribution coefficient k) and having a phase angle β_(W) is vector-added to the RFV primary component of the single tire unit and that the entire RFV primary component is formed. At this time, it should be noted that the phase of the RFV primary component of the single tire unit is added only at the assembling angle θ in the wheel system. The amplitude of the RFV primary component of the entire system which is the magnitude of the result of the vector addition is given by the formula (3) in the same way as in the case of the formula (2).

As described above, if the formulas (1), (2), and (3) are used, the amount of unbalance and the RFV primary component when the wheel and the tire are assembled in the arbitrary positional relationship (the assembling angle θ in FIG. 3) can be predicted as the function of the assembling angle θ.

When the tire and the wheel are assembled, a plurality of conditions are considered according to the demand of users as to how to balance the assembled tire and wheel unit. For example, the entire unbalance mass is reduced and corrected, or the RFV primary component amplitude is reduced and corrected, or these are combined and corrected, or the like. These conditions are determined as evaluation functions. Namely, the evaluation functions which match a purpose are determined and the assembling angle when the evaluation functions are optimized is obtained. In this way, the correction of unbalance which matches the purpose can be carried out.

General concrete examples of evaluation functions will be described below.

[Evaluation Functions]

(A) evaluation function=n₁+n₂

(B) evaluation function=n₁

(C) evaluation function=A n₁+B n₂+C f (A, B, C>0)

(D) (if f₀+kΔr<RFV reference value)

evaluation function=n₁+n₂

(E) (if f₀+kΔr≧RFV reference value, and μ₁+m₁+μ₂+m₂<amount of weight reference value)

evaluation function=f

(F) (if f₀+kΔr≧RFV reference value, and μ₁+m₁+μ₂+m₂≧amount of weight reference value)

evaluation function=evaluation function (C)

(G) evaluation function=amount of static unbalance after assembling

The evaluation function (A) evaluates amounts of unbalance weight to be corrected n₁ and n2 at the front and reverse sides of the wheel which is assembled with the assembling angle θ being a parameter. The evaluation function (B) evaluates an amount of unbalance weight to be corrected n₁ at the front side of the wheel which is assembled with the assembling angle θ being a parameter. The evaluation function (C) evaluates amounts of unbalance weight to be corrected n₁ and n₂ and the RFV primary amplitude f at the front and reverse sides of the wheel which is assembled with the assembling angle θ being a parameter. The evaluation function (D) evaluates amounts of unbalance weight to be corrected n₁ and n₂ at the front and reverse sides of the wheel which is assembled with the assembling angle θ being a parameter and only when f₀+kΔr<RFV reference value. The evaluation function (E) evaluates an RFV primary amplitude f only when f₀+kΔr≧RFV reference value and μ₁+m₁+μ₂+₂<amount of weight reference value. The evaluation function (F) evaluates the same as that of the evaluation function (C) only when f₀+kΔr≧RFV reference value and μ₁+m₁+μ₂+m₂≧amount of weight reference value. The evaluation function (G) evaluates an amount of static unbalance after the assembling with the assembling angle θ being a parameter.

In the above-described evaluation functions, when only the amount of unbalance weight to be corrected n₁ is minimized using the evaluation function (B), an optimum value θ* of the assembling angle can be obtained as π.

Further, when only the amplitude f of the RFV primary component is minimized using the evaluation function (E), the conventional RFV primary matching is effected, and an optimum value θ* of the assembling angle θ can be easily obtained by the following formula (8).

θ*=π−β_(T)+β_(W)  (8)

Moreover, when the amount of static unbalance after the assembling is minimized using the evaluation function (G), an optimum value θ* can be easily obtained by the following formula (9).

θ*=π+agr(μ₁+μ₂ cos α_(W), μ₂ sin α_(W))−agr(m ₁ +m ₂ cos α_(T), μ₂ sin α_(T))  (9)

wherein, agr (x, y) is an angle which is formed by a positional vector which links an origin point with coordinates (x, y) counterclockwisely from the x-axis.

In the above-described formula (9), the unbalance mass (μ₁, μ₂, m₁, m₂) exists as a parameter. However, these vector components are acted on by the optimum value θ*, and the value of each of the amounts of unbalance (the parameters on both surfaces) is not needed. As far as the magnitudes of unbalance of the tire and the wheel, i.e., the amount of static unbalance and the phase, are known, the optimum value θ* can be decided by the condition in which the phase of wheel's static unbalance and the phase of tire static unbalance are just 180 degrees opposite each other. Accordingly, as a simple concrete example, when only the amount of static unbalance and the phase are known, the above-described evaluation function (G) are effective. Namely, when the amounts of static unbalance of the tire and the wheel and the phase are known, the tire and the wheel are assembled so that the phase becomes π (180 degrees).

In the above-described evaluation functions (B), (E), and (G), the assembling angle θ can be easily obtained. However, in the other evaluation functions, the assembling angle θ which provides an optimum value of the evaluation function cannot be always obtained analytically. The assembling angle θ can be easily determined by numerical computation. Namely, if the necessary parameters are input using a spreadsheet program and numerical operation of a personal computer, it is easy to output a result instantly. Namely, degrees from 0 to 360 are divided into as many equivalent angles as the accuracy of the angle to be obtained requires, the evaluation function of each angle step is actually calculated, and an optimum value may be determined from the results, i.e., all of the calculated results.

Next, a description will be given of a system for obtaining a phase angle when a tire and a wheel are assembled on the basis of the aforementioned principle.

FIG. 4 shows a schematic view of a personal computer for effecting a method of assembling a tire and a wheel of the present invention. The personal computer comprises a keyboard 10 for inputting data or the like, a computer main body 12 which evaluates a phase angle at the time of assembling a tire and a wheel in accordance with a program stored in advance, and a CRT 14 which displays evaluation results or the like of the computer main body 12. The computer main body 12 is formed by a microcomputer comprising an unillustrated CPU, ROM, and RAM.

The computer main body 12 includes a recording medium which records a phase angle operating program at the time of assembling a tire and a wheel of the present invention, e.g., a floppy disk unit (FDU) 16 into/from which a floppy disk(FD) can be inserted/removed. A processing routine, which will be described later, or the like can be read from and written onto the FD using the FDU 16. Consequently, the processing routine, which will be described later, may be recorded onto the FD in advance without being recorded onto the unillustrated ROM in the computer main body 12 and execute a processing program recorded onto the FD via the FDU 16. A mass storage system (unillustrated) such as a hard disk device or the like may be connected to the computer main body 12 and the processing program recorded onto the FD may be installed in the mass storage system (unillustrated) and executed. Further, an optical disk such as a CD-ROM or the like and an optical magnetic disk such as an MD, MO, or the like exist as a the recording medium, and when these disks are used, a CD-ROM device, an MD device, an MO device, or the like may be used instead of the above-described FDU 16.

Next, a description will be given of a processing for obtaining a predicted angle which is an optimum angle among phase angles at the time of assembling a tire and a wheel.

As explained in the above principle, the present inventors have considered that the correction of unbalance to fulfil a purpose can be evaluated to be effected on the assembling of a tire and a wheel by predicting the amount of unbalance and the RFV primary component when the wheel and the tire are assembled in an arbitrary positional relationship (the assembling angle θ in FIG. 3) using the formulas (1) through (3) as a function of the assembling angle θ.

FIG. 5 shows a processing routine of a program of the present embodiment. In step 100, measured values are input. These measured values are an unbalance mass μ₁ at the front side of a single wheel unit, an unbalance mass μ₂ at the reverse side of the single wheel unit, a phase difference α_(W), a primary component amplitude Δr of a radial run-out of the single wheel unit, a phase angle β_(W), a contribution coefficient k, an unbalance mass ml at the front side of the single tire unit, an unbalance mass m₂ at the reverse side of the single tire unit, a phase difference α_(T), an RFV primary component amplitude f₀ of the single tire unit, and a phase angle β_(T).

In a subsequent step 102, evaluation functions which are explained above are determined. In the next step 104, an optimum assembling angle is determined as a predicted angle θ using the determined evaluation function and is output in the next step 106.

By effecting the assembling of the wheel and the tire at the assembling angle θ which is determined by various types of evaluation functions as described above, the present inventors have studied in simulation the assembled unit to be actually obtained.

First, a population model relating to dispersions of products of the wheel and the tire is assumed. In a condition to be expressed, the wheel has the three random vectors (μ₁, μ₂, kΔr), where μ₁ is the unbalance mass at the front side, μ₂ is the unbalance mass at the reverse side, and Δr is the primary component amplitude of radial run-out. The tire has the three random vectors (m₁, m₂, f₀), where m₁ is the unbalance mass at the front side, m₂ is the unbalance mass at the reverse side, and f₀ is the RFV primary component amplitude. These probability distributions are considered as follows for modeling.

First, when the starting point of the respective random vector distributions is placed on the origin point, the end point follows such distribution in which the X coordinate and the Y coordinate follow independently the same normal distribution (standard deviation σ) on the X-Y plane. By doing so, a probability distribution is formed in which the directions of vectors have the same probabilities in every direction and only the length exists. However, the distribution of length is known as a Rayleigh distribution, and the mean is {{square root over ( )}(π/2) σ} and a mean square value is 2σ². Thus, a standard random vector in which 2σ²=1 is assumed for vector e. When E ( ) is defined as the symbol of an expectation, the expectation of vector e can be expressed in the following formula (10).

E(e)=0

E(|e|)={square root over ( )}π/2

E(ee)=1  (10)

Accordingly, a random vector A in which the mean of a length is a can be expressed in the following formula (11).

A=(2/{square root over ( )}π)αe  (11)

Next, vector B which correlates to the vector A is considered. When β is the mean of a length, it can be expressed as B=(2/{square root over ( )}π) βe′ (wherein, vector e′ is a separate standard random vector which is not independent from the vector e). A correlation coefficient ρ of the two random vectors A and B is defined in the following formula (12).

ρ=E(AB)/[{square root over ( )}E(A ²){square root over ( )}E(B²)]  (12)

When the vectors A and B are definite vectors, since the correlation coefficient p is equal to the cosine of the angle formed by these directions, nearness between the directions of vectors is indicated. In this case, when the correlation coefficient ρ is expressed by the standard vector, the following formula (13) is formed.

ρ=E(ee′)  (13)

Here, e′=ρe+ce″ (wherein, vector e″ is another standard random vector which is independent from the vector e). When both sides of this definition formula are multiplied by the vector e and an expectation is obtained by using the result, the definition formula corresponds to the formula (13) in which the correlation coefficient of the vector e and the vector e′ is ρ. Further, because the expectation which is obtained by squaring both sides must be equal to 1, the value of c is determined as {square root over ( )}(1−ρ²). Next, a third vector C which correlates with the vectors A and B by correlation coefficients ρ′ and ρ″ is considered. In the same consideration as described above, when the third independent standard vector is introduced into the vector C, the vector C can be expressed by the linear combination of three standard vectors and the coefficients can be expressed as ρ, ρ′, and ρ″. Namely, models of random vectors A, B, C which correlate to each other can be expressed in the following formula (14). $\begin{matrix} \begin{matrix} {A = {\sqrt{E\left( A^{2} \right)}e_{1}}} \\ {B = {\sqrt{E\left( B^{2} \right)}\left\lfloor {{\rho \quad e_{1}} + {\sqrt{1 - \rho^{2}}e_{2}}} \right\rfloor}} \\ {C = {\sqrt{E\left( C^{2} \right)}\left\lfloor {{\rho^{\prime}e_{1}} + {\frac{\rho^{''} - {\rho\rho}^{\prime}}{\sqrt{1 - \rho^{2}}}e_{2}} + {\left( \sqrt{1 - \rho^{\prime 2} - \frac{\left( {\rho^{''} - {\rho\rho}^{\prime}} \right)^{2}}{1 - \rho^{2}}} \right)e_{3}}} \right\rfloor}} \end{matrix} & (14) \end{matrix}$

wherein, e₁, e₂, and e₃ are standard random vectors which are independent from each other. More specifically, in order to generate the vectors e₁, e₂, and e₃, the x component and the y component may be independent normal distribution random numbers whose standard deviation is (1/{square root over ( )}2).

Models of the above-described random vectors are applied to the vectors μ₁, μ₂, kΔr and the vectors m₁, m₂, and f₀. An example which studies optimization of various evaluation functions is shown in Tables 1 through 3 and FIGS. 6A through 6E.

TABLE 1 Wheel Variable kΔr ρ′ μ₁ ρ μ₂ ρ″ Population 2.0 0.7  7.0 0.5  7.0 0.3 mean Tire Variable f₀ ρ′ m₁ ρ m₂ ρ″ Population 8.6 0.5 15.0 0.4 15.0 0.6 mean

Tables 2 and 3 show means of simulation results of unbalance matching of the wheel and the tire.

TABLE 2 Strategy 1 Strategy 2 Minimalization of n₁ + n₂ Minimalization of n₁ RFV RFV n₁ n₁ + n₂ primary n₁ n₁ + n₂ primary Mean 11.19 21.11 7.77 Mean 9.24 23.60 7.82 Strategy 3 Strategy 4 RFV primary matching Random assembling RFV RFV n₁ n₁ + n₂ primary n₁ n₁ + n₂ primary Mean 14.64 29.10 6.23 Mean 16.85 32.42 8.64

TABLE 3 n₁ + n₂ RFV primary Minimalization of 21.11 7.77 n₁ + n₂ Minimalization of n₁ 23.60 7.82 RFV primary 29.10 6.23 matching Random Assembling 32.42 8.64

Table 1 shows a detail of the model of random vectors and Table 2 shows results to which the aforementioned evaluation functions are applied. Table 2 shows means when Strategies 1 through 3 and no strategy are effected using data in Table 1. Strategy 1 shows means of simulation results (values which will be obtained at the time of measurement are predicted) of the assembled unit in which the assembling angle θ is determined using the evaluation function A (minimalization of n₁ and n₂) and then the tire and the wheel are assembled. Further, Strategy 2 shows means of simulation results of the assembled unit in which the assembling angle θ is determined using the evaluation function B (minimalization of n₁) and then the tire and the wheel are assembled. Moreover, Strategy 3 shows means of simulation results of the assembled unit in which the assembling angle θ is determined using the evaluation function E (matching of RFV primary amplitude f) and then the tire and the wheel are assembled. No strategy shows means of simulation results of the assembled unit in which the assembling angle θ is determined at random and then the tire and the wheel are assembled.

FIGS. 6A through 6E show the dispersions in the above-described respective strategies. In FIGS. 6A through 6E, the simulation results of a plurality of assembled tire and wheel unit are shown as dispersions of dots with the abscissa being the total amount of unbalance weight to be corrected (n₁+n₂) at the front and reverse sides of the assembled wheel and the ordinate being an RFV primary amplitude f. FIG. 6A corresponds to Strategy 1 and shows the simulation results for an assembled unit in which the assembling angle θ is determined using the evaluation function A (minimalization of n₁ and n₂) and the tire and the wheel are then assembled. Further, FIG. 6B corresponds to Strategy 2 and shows the simulation results for an assembled unit in which the assembling angle θ is determined using the evaluation function B (minimalization of n₁) and the tire and the wheel are then assembled. Moreover, FIG. 6C corresponds to Strategy 3 and shows the simulation results for an assembled unit in which the assembling angle θ is determined using the evaluation function E (matching of RFV primary amplitude f) and the tire and the wheel are then assembled. FIG. 6D corresponds to no strategy and shows the simulation results for an assembled unit in which the assembling angle θ is determined at random without using the evaluation function and the tire and the wheel are then assembled.

Table 3 and FIG. 6E show the results regarding the above-described strategies.

The simulations effected as above are one example. An arbitrary value is given to a population parameter and data of a wheel and a tire (N=100) is generated and calculated by a random number. As a result, while the total amount of balance weight per one assembled unit by effecting the assembling in accordance with a conventional RFV primary matching is 29.1 g, it is predicted that the total amount thereof by effecting the assembling which minimizes the total amount of weight (n₁+n₂) will be reduced to 21.1 g. The ratio of reduction is approximately 27%, and thus the effect is large. In this case, the deterioration of RFV primary is 7.77 kgf from 6.23 kgf and the ratio of deterioration is about 25%. If this deterioration is within the permissible range, a strategy which reduces weight may be taken. Further, when only the assembling which minimizes the total amount of weight (n₁) at the front side is carried out, it is predicted that the total amount of weight (n₁+n₂) is reduced to 23.6 g and the ratio of reduction is approximately 20%. The actual magnitudes of these effects depend on the magnitude of the irregularities of each wheel and tire or the directionality thereof and are not determined absolutely. However, it is obvious that the statistical characteristics of the irregularities are effective as a means of providing procedures for optimum selection.

Example of the present invention will be described in detail hereinafter.

In accordance with the above-described simulations, the difference in amounts of unbalance to be corrected due to the difference in assemblings is actually experimented using wheels and tires (sample numbers N=20).

[Data of a Tire and a Wheel]

magnitude of tire: 205/65R15 20 wheel: 6JJ × 15 made of steel 20

First, in preparation for starting the experiment, the following items {circle around (1)} through {circle around (6)} were effected.

Item {circle around (1)}: The unbalance of each of 20 wheels was measured by a two-plane balancer and the above-described parameters μ₁, μ₂, and α_(W) were obtained. A mark was made at the position of the unbalance mass μ₁ at the front side.

Item {circle around (2)}: Radial direction vibrations of front and reverse bead bases of each of the 20 wheels were measured by a laser displacement meter and the average waveform of the waveforms of the front and reverse bead bases were subjected to Fourier analysis. The primary component amplitude Δr and its peak (the most protruding portion) phase angle β_(W) were obtained. A mark was made at the position (the lowest portion of vibrations) 180 degrees opposite the phase angle β_(W).

Item {circle around (3)}: The unbalance of each of 20 tires was measured by the two-plane balancer and the above-described parameters m₁, m₂, and α_(T) were obtained. A mark was made at the position of the unbalance mass m₁ at the front side.

Item {circle around (4)}: A single RFV of each of 20 tires was measured by a uniformity testing machine and an RFV primary component amplitude f₀ and the peak phase angle β_(T) were obtained. A mark was made at the position of the phase angle β_(T).

Item {circle around (5)}: Numbers 1 to 20 were given to each of the wheels and tires at random and the wheel and the tire having the same number were fixed as a pair for assembling.

Item {circle around (6)}: A pair No. 1 and a pair No. 2 were chosen and the position of phase angle β_(W) of the wheel in the above-described item {circle around (2)} and the RFV primary peak position (the position of β_(T)) of the tire in the above described item {circle around (4)} were combined and rim-assembled. The amplitude of the RFV primary component was obtained. Next, the wheel was rotated 180 degrees to the tire and reassembled, and the amplitude of the RFV primary component was measured in the same way. Since it is assumed from the model that the latter measured value is larger than the former measured value by 2 k Δr, half of the difference is divided by Δr and the contribution coefficient k is identified. The mean of the contribution coefficient k of the pairs No. 1 and No. 2 is 25.3 kgf/mm. This value was used for the No. 1 to No. 20 tires as a common value.

Table 4 shows the complete obtained parameters.

TABLE 4 # μ₁g μ₂g α_(w) Δr mm β_(w) m₁g m₂g α₁ f₀ kgf β_(T) 1 1 3 152 0.0980 225 4 11 313 5.6 2 2 0 7 220 0.0860 304 9 2 45 4.0 3 3 4 4 181 0.0602 43 31 26 9 7.1 335 4 9 4 152 0.0945 8 8 17 33 9.1 1 5 5 3 342 0.0529 8 5 3 1 2.9 156 6 5 9 14 0.0265 146 0 7 7 5.2 3 7 7 7 279 0.0825 88 17 17 4 6.0 5 8 2 0 33 0.0926 269 9 19 359 1.7 356 9 2 9 101 0.0319 356 5 14 17 5.6 8 10 12 15 13 0.1435 17 42 36 359 9.2 2 11 3 6 275 0.0741 67 16 16 13 5.5 1 12 8 8 0 0.1262 40 7 5 9 2.3 222 13 13 5 306 0.1413 359 8 6 355 0.8 357 14 4 8 283 0.0372 225 5 6 359 3.3 25 15 6 4 294 0.1289 38 5 4 226 6.3 280 16 4 5 304 0.0277 341 3 10 357 6.6 0 17 4 2 0 0.0311 132 7 3 2 8.6 9 18 7 2 134 0.0800 339 0 13 29 15.3 43 19 10 5 3 0.1228 36 23 19 7 9.9 3 20 5 8 3 0.0654 288 8 9 7 5.5 140

Next, as a result of optimizing the above-described representative evaluation functions using the above-described data, the results shown in Tables 5 through 8 were obtained.

TABLE 5 Minimalization of n₁ + n₂ Prediction Assem- Actual measurement Sample bling RFV RFV No. angle n₁ n₁ + n₂ primary n₁ n₁ + n₂ primary 1 25 14.8 21.9 3.2 14 21 3.4 2 180 1.3 19.8 6.0 1 20 5.5 3 207 27.3 56.9 16.0 27 51 15.1 4 181 1.3 20.0 7.5 1 20 7.1 5 159 9.9 11.8 3.9 10 12 4.1 6 148 6.4 9.1 5.4 7 8 5.6 7 138 12.2 25.1 7.4 12 25 7.8 8 209 16.7 25.9 13.0 17 26 12.4 9 260 15.0 19.7 6.4 14 20 6.9 10 188 29.5 50.6 6.9 29 47 6.9 11 102 15.8 27.0 6.9 16 26 6.4 12 178 0.4 6.1 5.5 0 6 5.3 13 167 5.4 17.7 7.5 6 19 7.4 14 118 4.7 12.7 13.4 5 12 14.4 15 188 1.1 13.8 8.0 1 16 7.8 16 134 10.2 15.0 5.9 10 14 6.1 17 189 3.3 13.9 8.8 3 14 8.8 18 186 3.3 16.9 14.7 3 15 14.6 19 182 13.1 26.8 6.8 12 26 6.3 20 141 5.0 6.2 7.2 5 6 6.5 Mean 9.8 20.8 8.0 9.7 20 7.9

TABLE 6 Minimalization of n₁ Prediction Assem- Actual measurement Sample bling RFV RFV No. angle n₁ n₁ + n₂ primary n₁ n₁ + n₂ primary 1 180 12.4 26.3 7.8 11 27 8.6 2 180 1.3 19.8 6.0 1 22 5.8 3 180 26.8 57.0 16.6 26 64 18.0 4 180 1.3 20.0 7.5 1 20 8.2 5 180 9.4 12.2 4.1 9 12 4.5 6 180 5.0 11.3 5.0 5 12 4.8 7 180 9.3 27.4 6.1 9 26 6.1 8 180 16.3 28.3 11.9 17 27 12.3 9 180 13.3 29.1 5.4 15 30 5.1 10 180 29.3 51.0 6.5 29 52 6.3 11 180 13.4 31.4 4.7 13 33 4.2 12 180 0.3 6.2 5.5 0 6 5.3 13 180 4.9 18.2 7.3 5 19 7.6 14 180 0.9 16.6 14.2 1 15 14.4 15 180 0.8 14.0 8.3 1 13 9.1 16 180 8.5 20.4 6.3 9 20 6.3 17 180 3.2 14.1 9.0 3 15 9.1 18 180 3.2 17.0 14.5 3 16 13.4 19 180 13.1 26.8 6.9 12 27 6.9 20 180 2.6 9.1 7.0 3 9 7.1 Mean 9 22.8 8.0 9 23 8.1

TABLE 7 RFV Primary Matching Prediction Assem- Actual measurement Sample bling RFV RFV No. angle n₁ n₁ + n₂ primary n₁ n₁ + n₂ primary 1 33 14.7 21.9 3.2 14 22 3.3 2 32 18.1 25.9 1.9 18 25 2.1 3 248 29.6 57.0 15.6 31 57 14.9 4 137 13.9 34.1 6.7 14 34 6.4 5 32 19.3 23.4 1.6 19 22 1.6 6 253 9.9 23.6 4.5 10 23 4.2 7 263 17.3 41.8 3.9 17 43 4.0 8 93 18.9 43.9 9.4 20 41 9.2 9 107 14.8 37.5 4.8 15 38 4.4 10 145 32.4 60.5 5.5 32 52 5.8 11 236 14.8 36.3 3.6 14 35 4.2 12 358 15.1 27.2 0.9 16 27 1.0 13 182 4.9 18.4 7.3 5 19 7.2 14 20 8.9 25.6 12.3 8 29 11.5 15 298 9.2 21.4 3.0 9 22 3.0 16 121 11.0 15.8 5.9 10 17 5.9 17 293 9.7 22.0 7.8 11 21 8.4 18 116 9.3 24.5 13.3 10 24 14.1 19 193 13.5 27.3 6.7 13 27 7.2 20 328 12.7 29.9 3.9 13 30 4.3 Mean 15 30.9 6.1 15 30 6.1

TABLE 8 Static Unbalance Matching Prediction Assem- Actual measurement Sample bling RFV RFV No. angle n₁ n₁ + n₂ primary n₁ n₁ + n₂ primary 1 340 14.8 23.0 4.6 14 24 4.3 2 114 10.4 26.5 4.3 10 28 4.3 3 120 29.0 58.0 18.1 24 62 19.4 4 171 3.3 22.5 7.2 3 23 7.7 5 163 9.7 11.8 3.9 10 12 4.3 6 166 5.3 9.9 5.2 5 10 4.2 7 137 12.2 25.1 7.4 12 25 7.7 8 206 16.6 25.9 12.9 17 26 11.3 9 261 15.0 19.7 6.4 14 18 7.4 10 188 29.5 50.6 6.9 29 51 6.7 11 113 15.2 27.1 6.7 16 25 6.4 12 162 2.4 6.7 5.4 2 6 6.4 13 168 5.3 17.7 7.4 5 17 7.7 14 127 4.1 12.9 13.6 4 12 13.6 15 178 0.9 14.1 8.4 1 14 8.5 16 137 10.0 15.0 5.9 10 14 6.9 17 193 3.4 14.0 8.8 3 14 8.5 18 180 3.2 17.0 14.5 3 18 14.9 19 181 13.1 26.8 6.8 12 25 7.4 20 159 3.5 7.1 7.2 3 7 7.4 Mean 10 21.6 8.1 10 22 8.3

The following Table 9 shows means which are the results of the experiment in the above embodiment in which the wheel and the tire (N=20) are assembled.

TABLE 9 Prediction Actual Measurement RFV RFV n₁ n₁ + n₂ primary n₁ n₁ + n₂ primary Minimali- 9.8 20.8 8.0 10 20 7.9 zation of n₁ + n₂ Minimali- 8.8 22.8 8.0  9 23 8.1 zation of n₁ RFV 14.9 30.9 6.1 15 30 6.1 primary matching Static 10 21.6 8.1 10 22 8.3 unbalance matching

As can be understood from this Table 9, it was confirmed that the predictions and the actual measurements were nearly the same and the optimization of evaluation functions in the prediction was actually realized.

As described hereinbefore, in accordance with the first aspect of the present invention, the tire and the wheel are assembled at the predicted angle obtained from the evaluation functions on the basis of the magnitude and the position of each of the amounts of unbalance of the tire and the wheel. Thus, even if iron whose specific gravity is smaller than that of lead which has been conventionally used is used, the amount of unbalance itself can be reduced. Accordingly, a superior effect is achieved in that unbalance can be corrected without increasing the volume of the iron used.

In accordance with the second aspect of the present invention, the predicted angle for assembling the tire and the wheel is obtained on the basis of the magnitude and the position of each of the amounts of unbalance on the axial direction end surfaces of the tire and the axial direction end surfaces of the wheel using the evaluation functions including the phase angle at the time of assembling the tire and the wheel, and the tire and the wheel are assembled at the predicted angle. Thus, even if iron whose specific gravity is smaller than that of lead which has been conventionally used is used, the amount of unbalance itself can be reduced. Accordingly, a superior effect is achieved in that unbalance can be corrected without increasing the volume of the iron used.

In accordance with the third aspect of the present invention, the magnitude of an amount of static unbalance to be corrected after the tire and the wheel are assembled is used for the evaluation function. Thus, a superior effect is achieved in that the predicted angle of the wheel and the tire which can reduce the magnitude of a balance weight can be obtained and that the magnitude of the balance weight for correcting the unbalance can be reduced by reducing the amount of unbalance to be corrected to as small an amount as possible.

In accordance with the fourth aspect of the present invention, the magnitude of at least one of the amounts of unbalance to be corrected on the axial direction end surfaces of the wheel after the tire and the wheel are assembled is used for the evaluation function. Thus, a superior effect is achieved in that the magnitude of the balance weight for correcting the unbalance can be reduced by reducing the amount of unbalance to be corrected to as small an amount as possible.

In accordance with the fifth aspect of the present invention, the physical amount of unbalance includes the physical amount relating to the radial direction vibrations of the tire and the physical amount relating to the radial direction vibrations of the wheel, and evaluation is made by the physical amounts relating to the radial direction vibrations of the tire and the wheel after the tire and the wheel are assembled. Thus, a superior effect is achieved in that it is easy to assemble the wheel and the tire in consideration of the reduction of RFV.

In accordance with the sixth aspect of the present invention, evaluation is made by the sum of the physical amount of the magnitude of at least one of the amounts of unbalance correction on the axial direction end surfaces of the wheel after the wheel and the tire are assembled and a weight is attached thereto, and the physical amount relating to the radial direction vibrations of the wheel and the tire after the wheel and the tire are assembled and a weight is attached thereto. Thus, a superior effect is achieved in that, since the relationship at the time of assembling of the wheel and the tire is properly evaluated by the linear sum of amounts of unbalance, a balance weight or the like can be made as small as possible and the optimum phase angle for assembling the wheel and the tire can be obtained.

In accordance with the seventh aspect of the present invention, evaluation is made in a predetermined relationship by the physical amount of the magnitude of at least one of the amounts of unbalance correction on the axial direction end surfaces of the wheel after the wheel and the tire are assembled and a weight is attached thereto, and the physical amount relating to the radial direction vibrations of the wheel and the tire after the wheel and the tire are assembled and a weight is attached thereto. Thus, a superior effect is achieved in that a balance weight or the like can be made as small as possible and that the more optimum phase angle can be obtained.

In accordance with the eighth aspect of the present invention, a superior effect is achieved in that the wheel, to which the valve for intaking air is attached, can be used and that the optimum phase angle for assembling the tire and the wheel, to which the actual valve for intaking is attached, can be obtained. 

What is claimed is:
 1. A computer-readable medium comprising computer-executable instructions, the instructions including the steps of: (a) based on an amount of unbalance and position thereof for each of a tire and a wheel, selecting a predetermined evaluation function that predicts and uses at least one of an amount of unbalance weight to be corrected at a side of an assembled tire and wheel, and amplitude of a radial force variation component; (b) predicting evaluation function values at a number of different phase angles between the tire and the wheel at the time of assembly, the phase angles ranging from 0° to 360° with predetermined intervals; and (c) determining an optimum phase angle for assembling the tire and wheel to one another based on values obtained in step (b).
 2. The computer-readable medium of claim 1, wherein step (a) includes selecting from a plurality of predetermined evaluation functions, comprising at least one evaluation function for minimizing a total amount of balance mass required for balancing the tire and wheel when assembled to one other, and another evaluation function for minimizing an amount of balance mass required for balancing on the tire and wheel front side when assembled to one another.
 3. The computer-readable medium of claim 1, further comprising determining a contribution coefficient for transmission of radial run-out based on tire type.
 4. The computer-readable medium of claim 3, wherein said determining a contribution coefficient is performed by comparison of coefficient values for tire types having similar specifications.
 5. The computer-readable medium of claim 1, wherein step (b) includes, at least if an analytical solution is unavailable for the evaluation function, using numerical computation to predict the evaluation function values.
 6. The computer-readable medium of claim 5, wherein the optimum phase angle is determined according to within a predefmed accuracy requirement.
 7. The computer-readable medium of claim 1, wherein said predetermined evaluation function predicts and utilizes at least one of an amount of unbalance weight to be corrected when the tire and wheel are assembled to one another, an amount of unbalance weight to be corrected at the tire and wheel front side, an amount of unbalance weight to be corrected at the tire and wheel reverse side, and an amplitude of a radial force variation component.
 8. A computer program product for use with a computer in balancing a tire and a wheel when assembled to one another, the computer product comprising a computer usable medium encoded with instructions which, when executed by computer, cause the computer to perform steps including: (a) obtaining inputs for unbalance measurement data for each of the tire and the wheel, the unbalance measurement data at least comprising phase, primary component amplitude information, and unbalance mass for each of the tire and the wheel; (b) receiving a selection from a plurality of criteria for determining an optimum angle for assembling the tire and the wheel to one another, the criteria including at least one of, when the tire and the wheel are assembled to one another, minimizing balance mass required for balancing, and minimizing a primary component of radial force variation; (c) selecting a function for determining the optimum angle based on the criteria received from a plurality of predefined evaluation functions; (d) predicting values of the selected function at a number of different phase angles between the tire and the wheel at the time of assembly, the phase angles ranging from 0° to 360° with predetermined intervals; (e) determining the optimum angle using the selected functions; and (f) outputting the optimum angle for assembling the tire and the wheel to one another according to the received criteria.
 9. The computer program product of claim 8, wherein in step (b), the criteria of reducing mass required for balancing comprises one of minimizing a total amount of balance mass required for balancing, and minimizing an amount of mass required on the tire and wheel front side for balancing.
 10. The computer program product of claim 8, wherein step (d) includes, at least if the optimum angle cannot be obtained analytically from the selected function, using numerical computation to determine the optimum angle.
 11. The computer program product of claim 10, wherein the optimum angle is determined to within a predefined accuracy requirement.
 12. The computer program product of claim 8, wherein in step (a), the unbalance measurement data includes tire type.
 13. The computer program product of claim 12, further comprising determining, based on tire type, a contribution coefficient for transmission of radial run-out.
 14. A computer program for use in balancing a tire and a wheel, the program embodied on a computer-readable medium and comprising instructions which, when executed by a computer, cause the computer to perform steps including: (a) obtaining inputs for unbalance measurement data for each of the tire and the wheel, as unassembled components; (b) selecting a function from a plurality of predetermined functions for determining an optimum positional relationship for when the tire and the wheel are assembled to one another, based on at least one of minimizing an amount of unbalance weight to be corrected in the assembled tire and wheel, and magnitude of a radial force variation primary component in the assembled tire and wheel; (c) predicting values of the selected function at a number of different phase angles between the tire and the wheel at the time of assembly, the phase angles ranging from 0° to 360° with predetermined intervals; (d) determining the optimum positional relationship using the selected functions; and (e) outputting the optimum positional relationship for assembling the tire and the wheel to one another.
 15. The computer program of claim 14, further comprising receiving an input for which basis to select the function.
 16. The computer program of claim 15, wherein the input for which basis to select is user entered during execution of the instructions by a computer.
 17. The computer program of claim 16, wherein step (b) includes at least one of minimizing a total amount of unbalance to be corrected in the assembled tire and wheel, minimizing unbalance to be corrected at only one side of the assembled tire and wheel, and minimizing magnitude of a radial force variation primary component in the assembled tire and wheel.
 18. The computer program of claim 14, wherein at least if the selected function requires use of a contribution coefficient for transmission of radial run-out, the inputs include tire specifications.
 19. The computer program of claim 18, further comprising determining the contribution coefficient based on the tire specifications, wherein the contribution coefficient is used by the selected function.
 20. The computer program of claim 14, where the step of determining the optimum positional relationship includes, at least if the optimum positional relationship cannot be obtained analytically from the selected function, using numerical computation to determine the optimum positional relationship. 